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Magnetismus Donnerstag resonante Mode auf, bei der die Position des Vortex auf einer Kreisbahn um den Mittelpunkt der Kreisscheibe mit der Frequenz des angelegten Felds rotiert [2]. Bei höherer Frequenz von ca. 5 GHz enteht eine resonante Mode anderen Typs, bei der stehende Wellen innerhalb der Kreisscheibe angeregt werden. [1] A. Wachowiak et al., Science 298, (5593) 577 (2002) [2] Guslienko et al., J. Appl. Phys. 91 (10) 8037 (2002) MA 28.5 Do 16:15 H23 Spin Dynamics in Permalloy Disks with Vortex Structure — •Matthias Buess 1,2 , Rainer Höllinger 1 , Thomas Haug 1 , Korbinian Perzlmaier 1 , Michael R. Scheinfein 3 , Danilo Pescia 2 , and Christian H. Back 1 — 1 Institut fürExperimentelle und Angewandte Physik, Universität Regensburg, Universitätsstrasse 31, 93040 Regensburg, Germany — 2 Laboratorium für Festkörperphysik,Eidgenössische Technische Hochschule Zürich, CH-8093Zürich,Switzerland — 3 Simon Fraser University, 8888 University Drive, Burnaby BC U5A 156, Canada Micron sized ferromagnetic permalloy disks exhibiting a ferromagnetic vortex structure are excited by a magnetic field pulse. The fast rise time pulse field is generated by an optically triggered electrical pulse in a lithographically fabricated microcoil. The excitation is imaged using time resolved magneto-optic polar Kerr microscopy - a stroboscopic experiment. We present the spatially resolved magnetic maps at different delay times, stitched together to form a magnetic movie. The dynamical excitations are composed of symmetric and non-sysmmetric parts which can not be separated at first glance. However, in the Fourier transformation of the magnetic movie we identify several modes which can be accounted for in a simple model based on purely dipolar interactions. The model is supported by micromagnetic simulations and shows good quantitative agreement in the resonance frequencies for different modes and sample dimensions. MA 28.6 Do 16:30 H23 NANOSECOND TIME-SCALE SWITCHING OF THIN FILM PERMALLOY ELEMENTS — •Dmitry Chumakov, Rudolf Schäfer, Jeffrey McCord, and Ludwig Schultz — IFW-Dresden, Helmholtzstr. 20, D-01069 Dresden, Germany We have studied the dynamic magnetization switching behaviour of thin film Permalloy elements by gated ICCD camera-based time-resolved wide-field Kerr microscopy. The structures were subject to pulsed magnetic fields of different strengths from 1600 A/m to 5200 A/m. Their reversal was observed with 250 ps time-resolution. By interpreting the experimental results we point out the peculiarities of the nanosecond timescale switching. Like in the quasistatic case, the dynamic remagnetization process is dominated by the generation of concertina-like domain patterns. Whereas such ”blocked” domains decay irreversibly in several steps during quasistatic switching, the blocking is resolved by continuous rotation in a locally inhomogeneous way for dynamic switching. This process lasts several nanoseconds and leads to significant delays in element switching. The influence of magnetic field amplitude, rise-time, and element shape on the switching behaviour will be shown at various examples. MA 28.7 Do 16:45 H23 Magnetization Dynamics of Micron Sized Permalloy Squares — •Korbinian Perzlmaier, Christian Back, Matthias Buess, and Rainer Höllinger — Institut für Experimentelle und Angewandte Physik, Universität Regensburg, Universitätsstrasse 31, 93040 Regensburg We investigate the dynamic response of the magnetization in micron sized Permalloy squares by measuring the polar Kerr component in a time resolved Kerr-microscope. The sample is excited with a fast rise time magnetic field pulse (typically pulse fields are smaller than 100 Oe) applied perpendicular to the sample plane. Magnetic movies are recorded with a frame rate of 10 ps. From the Fourier transform of the data we obtain information about the modal frequencies. Numerical methods based on the LLG equation are commonly used to simulate the dynamic response of magnetic elements. We extract the modal structure from simulated movies of squares in the size range between 300 nm and 4 micron. The results are compared to our experiments. MA 28.8 Do 17:00 H23 Investigation of magnetization dynamics of microstructured magnetic thin films by means of Time-Resolved Photoemission Electron Microscopy. — •A. Krasyuk 1 , A. Oelsner 1 , S.A. Nepijko 1 , D. Neeb 1 , A. Kuksov 2 , C.M. Schneider 2 und G. Schönhense 1 — 1 Johannes Gutenberg-Universität Mainz, Institut für Physik, Staudinger Weg 7, 55099 Mainz, Germany — 2 Institut für Festkörperforschung, Forschungszentrum Jülich, 52425 Jülich, Germany The magnetisation reversal dynamics of the lithographically prepared Permalloy particles with different forms and thickness ranging from 10nm up to 40nm was observed exploiting the Magnetic X-Ray Circular Dichroism (MXCD) contrast at the Ni L3 X-ray absorption edges in subns range by means Time-Resolved Photoemission Electron Microscope. The experiment has been performed in single-bunch mode at the BESSY II (Berlin) and 16-bunch mode at the ESRF (Grenoble). [1] A. Krasyuk, A. Oelsner, S.A. Nepijko, A. Kuksov, C.M. Schneider, G. Schönhense., Appl.Phys.A, 2003, 76, No.6, 863-868. [2] A. Oelsner, A. Krasyuk, D. Neeb, S.A. Nepijko, A. Kuksov, C.M. Schneider, G. Schönhense., J. Electr. Spectr. Rel. Phenom, accepted MA 28.9 Do 17:15 H23 Damping in thin NiFe films — •Hans Nembach, Markus C. Weber, Jürgen Fassbender, and Burkard Hillebrands — Fachbereich Physik und Forschungsschwerpunkt MINAS, Technische Universität Kaiserslautern, Erwin-Schrödinger-Str. 56, 67663 Kaiserslautern We investigated the damping and spin wave creation in thin NiFe films with time-resolved magneto-optic Kerr effect magnetometry for small and large angle excitations. To gain further insight in the underlying damping process we employ a special measurement procedure, which allows us to determine all three magnetization vector components and therefore the length of the magnetization vector. A reduction of the magnitude of the magnetization vector indicates the creation of spin waves. These spin waves can be created directly by the stripline or by multi-magnon processes. The experimentally determined magnetization trajectory is compared with numerical simulations based on the Landau-Lifshitz equation, and the damping constant is extracted from these simulations MA 28.10 Do 17:30 H23 Dependence of magnetization reversal dynamics on magnetic anisotropy and interlayer coupling — •K. Fukumoto 1 , W. Kuch 1 , J. Vogel 2 , J. Camarero 3 , S. Pizzini 2 , Y. Pennec 2 , F. Offi 1 , M. Bonfim 4 , A. Fontaine 2 , and J. Kirschner 1 — 1 Max-Planck-Institut für Mikrostrukturphysik, Weinberg 2, D-06120 Halle, Germany — 2 Laboratoire Louis Néel, CNRS, 25 Avenue des Martyrs, B. P. 166, F-38042 Grenoble Cedex 9, France — 3 Dpto. Física de la Materia Condensada, Universidad Autónoma de Madrid, E-28049 Madrid, Spain — 4 Departamento de Engenharia Elètrica, Universidade do Paraná, CEP 81531-990, Curitiba, Brazil Time- and element-resolved magnetic domain imaging measurements were performed using x-ray magnetic circular dichroism photoelectron emission microscopy (XMCD-PEEM). Two types of spin-valve-like samples (Fe20Ni80/Cu/Co) were used in this study, one with and one without magnetic anisotropy in the film plane. Magnetization reversal during nanosecond-short magnetic field pulses was investigated by a pumpprobe technique. Domain wall motion induced by the field pulses (pump) was imaged using photon pulses from single bunch operation of BESSY (probe). Magnetization reversal and domain structure of the permalloy layer in the sample showing no anisotropy in the plane are strongly influenced by local pinning. In the sample with in-plane anisotropy, domain patterns during the reversal of the permalloy layer are less reproducible, and more influenced by the local coupling with the Co layer. Reversal mechanism, speed of domain wall motion, and the effect of magnetic interlayer coupling were also studied using single-pulse measurements. MA 28.11 Do 17:45 H23 All optical probe of coherent spin waves in exchange bias systems — •B. Beschoten 1 , A. Tillmanns 1 , S. Oertker 1 , G. Güntherodt 1 , I.K. Schuller 2 , C. Leighton 3 , and J. Nogués 4 — 1 2. Physikalisches Institut, RWTH Aachen, 52056 Aachen — 2 Department of Physics, UC San Diego — 3 Department of Chemical Engineering and Materials Science, University of Minnesota — 4 Departament de Fisica, Universitat Autònoma de Barcelona Time-resolved Kerr rotation is used to generate and to probe coherent spin waves in exchange biased ferro-/antiferromagnetic bilayer films of
Magnetismus Donnerstag Fe/MnF2. The exchange bias results from an unidirectional anisotropy which is established below the Néel temperature of the antiferromagnetic layer and can be identified as a shift of the magnetic hysteresis loop. In time-resolved Kerr rotation, an ultrashort laser pump pulse generates an unidirectional anisotropy field pulse which triggers coherent precession of the magnetization in the ferromagnetic layer. This coherent precession is monitored by a time-delayed laser probe pulse yielding a quantitative method to study magnetic anisotropy, ultrafast switching and damping phenomena. Work supported by DFG through SPP 1133, grant no. BE 2441/2-1 MA 28.12 Do 18:00 H23 Evidence of spin-pumping effect in the FMR of coupled trilayers — •T. Toliński 1,2 , K. Lenz 1 , J. Lindner 1,3 , E. Kosubek 1 , and K. Baberschke 1 — 1 Institut für Experimentalphysik, Freie Universität Berlin, Arnimallee 14, 14195 Berlin, Germany — 2 Permanent address: Institute of Molecular Physics, PAS, Smoluchowskiego 17, 60-179 Poznań, Poland — 3 New address: Institut für Physik, Universität Duisburg-Essen, Lotharstr. 1, 47048 Duisburg, Germany The spin dynamics between two ultrathin ferromagnetic layers (Ni, Co) exchange coupled via a nonmagnetic Cu spacer of a few monolayers is studied using in situ ferromagnetic resonance. The angular and the temperature dependence of the linewidth shows pronounced changes that can be understood assuming the presence of an additional Gilbert damping resulting from a spin-current pumped through the interface between the ferromagnetic and nonmagnetic layers and by considering the dynamical part of the interlayer exchange coupling. In contrast to investigations on Fe films decoupled by thick Au spacers [1] the effect of the interlayer exchange coupling on this phenomenon is presented here. The competition between the Gilbert damping inherent in the ferromagnetic film and the Gilbert damping developed by the interface leads to an irregular behavior of the temperature dependence of the resonance linewidth for both the in-phase and out-of-phase precessing modes. It is shown that the oscillatory nature of the coupling is also revealed in the dependence of the resonance linewidth ∆H on the spacer thickness. Supported by the DFG (Sfb 290, TP A2). [1] B. Heinrich et al., Phys. Rev. Lett. 90, 187601 (2003). MA 28.13 Do 18:15 H23 Comparison of Network Analyzer Ferromagnetic Resonance (NA-FMR) with pulsed inductive Measurements — •Ingo Neudecker 1 , Georg Woltersdorfer 2 , Matthias Buess 1 , Christian Back 1 , and Bret Heinrich 2 — 1 Fakultaet fuer experimentelle und angewandte Physik, Universitaet Regensburg, Universitaetstrasse 31, 93044 Regensburg — 2 Simon Fraser University, 8888 University Drive, Burnaby, British Columbia V5A-1S6, Canada MA 29 Hauptvortrag Nielsch We placed a 20 ML thick Fe film on top of a lithographically fabricated coplanar waveguide. In a 20 GHz high frequency setup the ferromagnetic system was excited first with a continuous sinusoidal excitation using a Vector Network Analyzer and second without changing the setup with a field pulse (pulse generator with 70 ps rise time) using a 20 GHz sampling Oscilloscope to detect the signal. By means of the resonance line one obtains from the NA-FMR both the resonance frequency from its position and the damping constant from its width. From the pulsed inductive measurement one extracts the resonance frequency using Fourier transformation and the damping constant from the decay of the observed oscillations. Varying the magnetic bias field one can consequently derive the resonance behavior for the two methods. Our purpose was to compare the fairly new NA-FMR method with its excellent signal to noise ratio which yields data in the frequency domain with the pulsed inductive measurement providing a time domain access to the resonance properties of the system. MA 28.14 Do 18:30 H23 Coherent magnetization dynamics on Gd(0001) at 3 THz and its temperature dependence — •Uwe Bovensiepen, Alexey Melnikov, Ilie Radu, Oleg Krupin, Kai Starke, Eckart Matthias, and Martin Wolf — Freie Universität Berlin, Fachbereich Physik, Arnimallee 14, 14195 Berlin Resonant absorption of femtosecond laser pulses at the exchange split surface state of Gd(0001) excites coherent optical phonons, which lead to a periodic modulation of the distance between surface and subsurface layer with a frequency of 3 THz [1]. This vibration has been investigated in situ by time-resolved second harmonic (SH) generation on Gd(0001) films grown in ultrahigh vacuum on W(110). The magnetic SH contribution has been extracted by analysis of the SH yield for opposite magnetization directions. As a function of pump-probe delay a modulation of the surface magnetization at 3 THz is detected, which is attributed to a modulation of the exchange coupling due to the lattice vibration. We suggest, that this quasi-instantaneous phonon-magnon coupling is observed near the surface due to a crossing of phonon and magnon dispersion relations. As a function of temperature the lattice and the magnetic oscillation amplitude decrease and vanish near the Curie temperature. Coherent bulk dynamics is observed by transient reflectivity at 10% higher frequency. These modes are excited due to coupling of the subsurface region to the surface vibration. [1] A. Melnikov et al.; Phys. Rev. Lett., (2003) in press. Zeit: Freitag 10:15–10:45 Raum: H10 Hauptvortrag MA 29.1 Fr 10:15 H10 Ferromagnetische Nanostäbe und Nanoröhren in selbstgeordneten Aluminiumoxid-Membranen — •Kornelius Nielsch — BMBF-Nachwuchsgruppe für Multifunktionale Nanostäbe und Nanoröhren, Max-Planck-Institut für Mikrostrukturphysik, Halle Die potentiellen Anwendungsgebiete für magnetische Nanoröhren und Nanostäbe reichen von Biotechnologie zu MRAMs. Aufgrund der potentiellen Anwendung als Datenspeicherung haben magnetische Nanostabensembles eine besondere wissenschaftliche Aufmerksamkeit in jüngster Zeit erfahren. Als Formstruktur wurden bienenwabenförmige Al2O3- Membranstrukturen zur Herstellung der Ni-, Fe- oder Co-Stabensembles mit periodischen Abständen von 65 nm und 100 nm und Durchmessern von 25 bis 55 nm verwendet. Aufgrund von Selbstorganisation sind die Nanostäbe hexagonal im 2D-Gittern quasi polykristallin angeordnet. Vor allem Nickel-Nanostabensemles zeigten eine geringe Dipolwechselwirkung im Ensemble und wurden intensiv mit SQUID-Magnetometer und MFM charakterisiert. Mittels Imprint-Lithographie konnten großflächig perfekt geordnete Stabensembles erzeugt werden. Ferner wurden mittels Brillouin-Lichstreuung quantisierte Energiezustände in den Magnetstäben nachgewiesen. Durch Polymerbeschichtung der Membranwände konnten Kobalt-Nanoröhren mit einer Wandstärke von 5 bis 20 nm und einem Durchmesser von 200 bis 500 nm hergestellt werden. Diese Arbeit fand in Zusammenarbeit mit den Arbeitsgruppen von Prof. C.A. Ross (MIT, Boston, USA), Prof. H. Kronmüller (MPI-Stuttgart), Prof D. Weiss (Uni Regensburg) und Prof. M.H. Kuok (National Universität Singapur) statt.
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Page 503 and 504:
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Symposium Physics of Foams Mittwoch
Page 509 and 510:
Symposium Physics of Foams Mittwoch
Page 511 and 512:
Symposium Quantum Shot Noise in Nan
Page 513 and 514:
Symposium X-RAY Magneto-Optics Tage
Page 515 and 516:
Symposium X-RAY Magneto-Optics Dien
Page 517 and 518:
Lehrertage Regensburg Hauptvorträg
Page 519 and 520:
A. D., Mirlin .................HL 1
Page 521 and 522:
Breidenbach, Boris ........ AKB 50.
Page 523 and 524:
Elli, Alexandra .............SYLS 3
Page 525 and 526:
Greer, Lindsay ......... M 9.1, M 1
Page 527 and 528:
Horn-von Hoegen, M. O 13.2, O 14.40
Page 529 and 530:
Korn, Tobias ...............MA 13.6
Page 531 and 532:
Martin, Tobias ............. MA 13.
Page 533 and 534:
Partyka, Ewa ................ M 18.
Page 535 and 536:
Rugeramigabo, Eddy Patrick O 14.38,
Page 537 and 538:
Sihler, J. .................... DS
Page 539 and 540:
Volz, K. .................... HL 44
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